Zoom lens system and optical apparatus using the same

ABSTRACT

There are provided a zoom lens system including, in order from an object side, a front lens component including a plurality of lens unit for zooming and focusing, and a rear lens component for forming an image, the rear lens is a zoom lens including, in order from the object side, a lens unit A of positive refractive power, a lens unit B of negative refractive power movable so as to have a component in a direction perpendicular to an optical axis for displacing the image, and a lens unit C of positive refractive power.

BACKGROUND OF THE INVENTION

[0001] The present invention relates to a zoom lens system and optical apparatus using the same, and more particularly those suitable for video cameras, digital cameras, and cameras using a silver halide film which attempt to stabilize a shot image and to optically correct blurs in the shot image when a zoom lens vibrates and tilts.

[0002] An image pick-up system having a long focal length, such as a telephoto lens, is generally so bulky and heavy that it is difficult to stabilize an image for such an image pick-up system. As the image pick-up system vibrates and tilts, a shot image displaces (or blurs) according to the tilt angle and the focal length of the image pick-up system. Thus, various image stabilizing optical systems have conventionally been proposed so as to prevent blurs in short images.

[0003] Generally speaking, a diameter and weight in an image stabilizing lens unit are important factors to obtain good image stabilization for large-aperture, telescope type zoom lenses. A large-aperture image stabilizing lens unit would require a large-caliber actuator for driving it, and lens's heavy weight would result in increased power consumption.

[0004] For example, an image stabilizing zoom lens proposed in Japanese Laid-Open Patent Application No. 8-278445 would possibly increase a diameter of image stabilizing lens unit. An image stabilizing zoom lens proposed in Japanese Laid-Open Patent Application No. 9-325269 uses two lenses to reduce image stabilizing lens unit's weight, and would possibly lead to aberrational fluctuations in stabilizing an image.

[0005] A mechanism for vibrating part of lens unit in an image pick-up system and for eliminating blurs in a static shot image generally requires a larger image-blur correction amount, smaller mobile and rotary amounts of a (movable) lens unit to be vibrated for blur corrections, a smaller size for the whole apparatus, and the like.

[0006] In addition, where the defocus of the movable lens unit causes much decentering aberration, the decentering aberration defocuses images after blurs are corrected. Therefore, an optical system having the image stabilizing function requires a smaller amount of decentering aberration to be generated when the movable lens unit is moved in a direction orthogonal to the optical axis and made in a decentering state.

BRIEF SUMMARY OF THE INVENTION

[0007] Accordingly, it is a primary but exemplified object of the present invention to provide a zoom lens system and an optical apparatus using the same, where the zoom lens system has a large aperture but includes such an image stabilizing system having a lightweight and small-diameter image stabilizing lens unit as provides a good optical performance in stabilizing an image, and maintains the entire apparatus compact.

[0008] In order to achieve the above object, a zoom lens system of one aspect according to the present invention includes, in order from an object side, a front lens component including, a plurality of lens units for zooming and focusing, and a rear lens component, as a relay lens unit, for forming an image, wherein the rear lens component including, in order from the object side, a lens unit A of positive refractive power, a lens unit B of negative refractive power movable so as to have a component in a direction perpendicular to an optical axis, and a lens unit C of positive refractive power, the image being displaced as the lens unit B moves so as to have the component in the direction perpendicular to an optical axis. According to this zoom lens system, a beam emitted from the front lens component converges by the lens unit A of relatively large positive refractive power, reduces an axial beam incident upon the lens unit B as an image stabilizing lens unit, and thereby reduces a lens diameter of the lens unit B. The lens unit B has relatively large refractive power to increase the image stabilizing sensitivity, while the lens unit C has relatively large positive refractive power and corrects an aberration generated by the lens unit B of relatively large negative refractive power. Thereby, the inventive zoom lens may miniaturize the entire apparatus and maintain a high optical performance throughout the entire zoom range or the entire object length in both reference and image stabilizing states.

[0009] The above zoom lens system may satisfy conditions −2.5<f5A/f5B<−1.0, −2.5<f5C/f5B<−1.0 and 1.0<f5B/fw<−0.1 where f5A, f5B, and f5C are focal lengths of the lens units A, B and C, respectively, and fw is a focal length of an entire lens system at wide-angle end. The upper equation indicates an optical power ratio between the lens unit A and the image stabilizing lens unit B in the rear lens component as an image forming lens system. The weaker power of the lens unit A beyond the upper limit value would increase the lens diameter of the lens unit B, thereby hampering the miniaturization of the image stabilizing lens unit B and deteriorating the aberrational balance with the lens unit B, in particular, a canceling performance of the spherical aberration. On the other hand, the stronger power of the lens unit A beyond the lower limit would facilitate the miniaturization of the lens unit B but deteriorate the aberrational balance, thereby leading to insufficient correction to the spherical aberration. The intermediate equation indicates an optical power ratio between the lens unit C and the image stabilizing lens unit B in the rear lens component. The weaker power of the lens unit C beyond the upper limit value would result in an excessive correction to the spherical aberration generated in the lens unit B, whereas the stronger power of the lens unit C beyond the lower limit value would result in an insufficient correction of the spherical aberration generated in the lens unit B. The lower equation relates power of the image stabilizing lens unit B. The weaker power of the lens unit B beyond the upper limit value would advantageously correct aberrations in stabilizing an image, but result in such a large lens diameter and a large mobile amount in the direction perpendicular to the optical axis in stabilizing an image due to the lowed power that the mechanical burden increases. On the other hand, the stronger power of the lens unit B beyond the lower limit value might reduce the lens diameter, and the mobile amount in the direction perpendicular to the optical axis in stabilizing an image, but deteriorate the spherical aberration and astigmatism.

[0010] The lens unit B may include one or more positive lenses and two or more negative lenses, thereby maintaining large optical power, decreasing the moving amount in the direction perpendicular to the optical axis in stabilizing an image, and facilitating a good optical performance.

[0011] The front lens component includes, in order from the object side, a first lens unit of positive refractive power, a second lens unit of positive or negative refractive power, a third lens unit of negative refractive power, and a fourth lens unit of positive refractive power, wherein during zooming from a wide-angle end to a telephoto end, a separation between the first and second lens units keeps constant or increases, a separation between the second and third lens units increases, and a separation between the third and fourth lens units changes. Thus, during zooming, the magnification is increased by moving the third lens unit of negative refractive power towards the image side, and resultant fluctuations of an image point is corrected by primarily moving the fourth lens unit of positive refractive power. The second lens unit used as a focus unit reduces a height of incidence of the axial beam, and reduces focus lens's diameter.

[0012] The second lens unit may move along the optical axis for focusing, thereby providing a good optical performance.

[0013] The first lens unit and rear lens component may be fixed during zooming from a wide-angle end to a telephoto end, thereby providing the good optical performance.

[0014] The zoom lens system may satisfy a condition Bf/ft>0.25 where Bf is a distance from a vertex in a lens surface at an image side of a lens closest to the image to an image plane, and ft is a focal length of an entire lens system at a telephoto end. This equation indicates a ratio of a distance from a vertex in the image-side surface of the lens closest to the image side to the shot surface relative to the focal distance of the entire lens system at the telephoto end. According to this zoom lens system, the focal distance ft exceeding the lower limit value would make difficult the attachment, for example, between the lens body and the camera body.

[0015] An optical apparatus of still another aspect according to the present invention includes the aforementioned zoom lens system and a photoelectric conversion element for receiving an image formed by the zoom lens system.

[0016] Other objects and further features of the present invention will become readily apparent from the following description of preferred embodiments with reference to accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

[0017]FIG. 1 shows lens sectional view of a zoom lens system at a wide-angle end of numerical example 1 according to the present invention.

[0018]FIG. 2 shows lens sectional view of the zoom lens system at a telephoto end of the numerical example 1.

[0019]FIG. 3 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 1 when the zoom lens system focuses on an infinite distant object.

[0020] FIGS. 4(A) and 4(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 1 which focuses on an infinite distant object, where FIG. 4(A) represents a normal state while FIG. 4(B) represents a state where the zoom lens stabilizes an image with an optical axis tilted by 0.5° from the normal state.

[0021]FIG. 5 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 1 when the zoom lens system focuses on an infinite distant object.

[0022] FIGS. 6(A) and 6(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system the numerical example 1 which focuses on an infinite distant object, where FIG. 6(A) represents the normal state while FIG. 6(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0023]FIG. 7 shows lens sectional view of a zoom lens system at a wide-angle end of numerical example 2 according to the present invention.

[0024]FIG. 8 shows lens sectional view of the zoom lens system at a telephoto end of the numerical example 2.

[0025]FIG. 9 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 2 when the zoom lens system focuses on an infinite distant object.

[0026] FIGS. 10(A) and 10(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 2 which focuses on an infinite distant object, where FIG. 10(A) represents the normal state and FIG. 10(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0027]FIG. 11 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 2 when the zoom lens system focuses on an infinite distant object.

[0028] FIGS. 12(A) and 12(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system of the numerical example 2 which focuses on an infinite distant object, where FIG. 12(A) represents the normal state and FIG. 12(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0029]FIG. 13 shows lens sectional view of a zoom lens system at a wide-angle end of numerical example 3 according to the present invention.

[0030]FIG. 14 shows lens sectional view of the zoom lens system at a telephoto end of the numerical example 3.

[0031]FIG. 15 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 3 when the zoom lens system focuses on an infinite distant object.

[0032] FIGS. 16(A) and 16(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 3 which focuses on an infinite distant object, where FIG. 16(A) represents the normal state and FIG. 16(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0033]FIG. 17 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 3 when the zoom lens system focuses on an infinite distant object.

[0034] FIGS. 18(A) and 18(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system of the numerical example 3 which focuses on an infinite distant object, where FIG. 18(A) represents the normal state and FIG. 18(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0035]FIG. 19 shows lens sectional view of a zoom lens system at a wide-angle end of numerical example 4 according to the present invention.

[0036]FIG. 20 shows lens sectional view of the zoom lens system at a telephoto end of the numerical example 4.

[0037]FIG. 21 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 4 when the zoom lens system focuses on an infinite distant object.

[0038] FIGS. 22(A) and 22(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 4 which focuses on an infinite distant object, where FIG. 22(A) represents the normal state and FIG. 22(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0039]FIG. 23 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 4 when the zoom lens system focuses on an infinite distant object.

[0040] FIGS. 24(A) and 24(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system of the numerical example 4 which focuses on an infinite distant object, where FIG. 24(A) represents the normal state and FIG. 24(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0041]FIG. 25 is schematic view of a principal part in an optical apparatus using the zoom lens system according to the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0042]FIGS. 1 and 2 show lens sectional view of a zoom lens system at wide-angle and telephoto ends, respectively, of numerical example 1, which will be described later. FIG. 3 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 1, which focuses on an infinite distant object. FIGS. 4(A) and 4(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 1 which focuses on an infinite distant object, where FIG. 4(A) represents a normal state while FIG. 4(B) represents a state where the zoom lens stabilizes an image with an optical axis tilted by 0.5° from the normal state. FIG. 5 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 1 when the zoom lens system focuses on an infinite distant object. FIGS. 6(A) and 6(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system the numerical example lwhich focuses on an infinite distant object, where FIG. 6(A) represents the normal state while FIG. 6(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0043]FIGS. 7 and 8 show lens sectional view of a zoom lens system at wide-angle and telephoto ends, respectively, of numerical example 2, which will be described later. FIG. 9 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 2, which focuses on an infinite distant object. FIGS. 10(A) and 10(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 2 which focuses on an infinite distant object, where FIG. 10(A) represents the normal state and FIG. 10(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state. FIG. 11 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 2 when the zoom lens system focuses on an infinite distant object. FIGS. 12(A) and 12(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system of the numerical example 2 which focuses on an infinite distant object, where FIG. 12(A) represents the normal state and FIG. 12(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0044]FIGS. 13 and 14 show lens sectional view of a zoom lens system at wide-angle and telephoto ends, respectively, of numerical example 3, which will be described later. FIG. 15 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 3, which focuses on an infinite distant object. FIGS. 16(A) and 16(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 3 which focuses on an infinite distant object, where FIG. 16(A) represents the normal state and FIG. 16(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state. FIG. 17 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 3 when the zoom lens system focuses on an infinite distant object. FIGS. 18(A) and 18(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system of the numerical example 3 which focuses on an infinite distant object, where FIG. 18(A) represents the normal state and FIG. 18(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0045]FIGS. 19 and 20 show lens sectional view of a zoom lens system at wide-angle and telephoto ends, respectively, of numerical example 4, which will be described later. FIG. 21 shows graphic representations of aberrations in the zoom lens system at the wide-angle end of the numerical example 4, which focuses on an infinite distant object. FIGS. 22(A) and 22(B) respectively show graphic representations of aberrations at the wide-angle end in the zoom lens system of the numerical example 4 which focuses on an infinite distant object, where FIG. 22(A) represents the normal state and FIG. 22(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state. FIG. 23 shows graphic representations of aberrations in the zoom lens system at the telephoto end of the numerical example 4 when the zoom lens system focuses on an infinite distant object. FIGS. 24(A) and 24(B) respectively show graphic representations of aberrations at the telephoto end in the zoom lens system of the numerical example 4 which focuses on an infinite distant object, where FIG. 24(A) represents the normal state and FIG. 24(B) represents the state where the zoom lens has the optical axis tilted by 0.5° from the normal state.

[0046] In a lens sectional view in each numerical example, G1 is a front lens component including a plurality of lens units for zooming and focusing. G2 is a rear lens component, as a rely lens, for forming an image.

[0047] The front lens component G1 includes, in order from an object side, first lens unit g1 of positive refractive power, second lens unit g2 of positive or negative refractive power, third lens unit g3 of negative refractive power, and fourth lens unit g4 of positive refractive power. During zooming from a wide-angle end (with the shortest focal length) to a telephoto end (with the longest focal length), the second, third and fourth lens units g2, g3, and g4 are moved as in arrows in the lens sectional view such that a separation between the first and second lens units g1 and g2 keeps constant or increases, a separation between the second and third lens units g2 and g3 increases, and a separation between the third and fourth lens units g3 and g4 changes.

[0048] The rear lens component G2 includes, in order from the object side, a lens unit g5A (or lens unit A) of positive refractive power which does not move in the direction perpendicular to the optical axis, a lens unit g5B (or lens unit B) of negative refractive power which may be moved in the direction perpendicular to the optical axis so as to correct blurs in an image when the zoom lens vibrates, and a lens unit g5C (or lens unit C) of positive refractive power which does not move in the direction perpendicular to the optical axis. Focusing associates with the movement of the second lens unit g2 in the optical axis direction. SP is an aperture stop, and IP is an image plane.

[0049] The zoom lens in this embodiment moves the third lens unit g3 of negative refractive power is moved toward the image side during zooming so as to increase the magnification, and corrects resultant fluctuations of an image point by primarily moving the fourth lens unit g4 of positive refractive power.

[0050] A description will now be given of the lens unit G1 including a plurality of lens units for zooming and focusing.

[0051] The zoom lens in this embodiment reduces the weight of the second lens unit g2 as the focus lens unit for auto focus purposes. In the known front (first unit) focusing, when the front weight becomes heavy in such a large-aperture lens system as the F-number of 2.8 and the close range is set to be as relatively short as about 1.5 m, the drawing amount for the focus lens unit disadvantageously becomes large. In addition, the spherical aberration particularly increases resulting in the insufficient correction at close range at the telephoto end, as the front lens's power (i.e., refractive power) becomes strong to reduce the drawing amount of the focus lens unit. Accordingly, the instant embodiment uses the second lens unit as the focus unit and reduces a diameter of the focus lens by diminishing a beam of incidence on the axial beam.

[0052] A description will now be given of the rear lens component G2 for forming an image. A beam emitted from the front lens component G1 converges through the lens unit g5A of relatively strong positive power, and diminishes the light incident upon the lens unit g5B as an image stabilizing lens unit on the axial beam. The lens unit g5B has larger refractive power to increase the image stabilizing sensitivity, while the lens unit g5C has relatively large positive power so as to correct an aberration generated by the lens unit g5B of large negative power.

[0053] The instant embodiment thus configures the lens units and obtains a high optical performance in both reference or normal and image stabilizing states throughout the zooming range or entire object length.

[0054] The zoom lens system of the instant embodiment may adopt at least one of the following configurations to obtain a better optical performance:

[0055] (a-1) The following equations are satisfied:

−2.5<f5A/f5B<−1.0   (1)

−2.5<f5C/f5B <−1.0   (2)

−1.0<f5B/fw<−0.1  (3)

[0056] where f5A, f5B, and f5C are focal lengths of the lens units A, B and C, respectively, and fw is a focal length of the entire lens system at wide-angle end.

[0057] The equation (1) indicates an optical power ratio between the lens unit g5A and the image stabilizing lens unit g5B in the rear lens component G2 as an image forming lens system. The weaker power of the lens unit g5A beyond the upper limit value would increase the lens diameter of the lens unit g5B, thereby hampering the miniaturization of the image stabilizing lens unit g5B and deteriorating the aberrational balance with the lens unit g5B, in particular, a canceling performance of the spherical aberration. On the other hand, the stronger power of the lens unit g5A beyond the lower limit would facilitate the miniaturization of the lens unit B but deteriorate the aberrational balance, thereby leading to insufficient correction to the spherical aberration.

[0058] The equation (2) indicates an optical power ratio between the lens unit g5C and the image stabilizing lens unit g5B in the rear lens component G2. The weaker power of the lens unit g5C beyond the upper limit value would result in an excessive correction to the spherical aberration generated in the lens unit g5B, whereas the stronger power of the lens unit C beyond the lower limit value would result in an insufficient correction of the spherical aberration generated in the lens unit g5B.

[0059] The equation (3) relates power of the image stabilizing lens unit g5B. The weaker power of the lens unit g5B beyond the upper limit value would be advantageously correct aberrations in stabilizing an image, but result in such a large lens diameter and a large mobile amount in the direction perpendicular to the optical axis in stabilizing an image due to the lowed power that the mechanical burden increases. On the other hand, the stronger power of the lens unit g5B beyond the lower limit value might reduce the lens diameter, and the mobile amount in the direction perpendicular to the optical axis in stabilizing an image, but deteriorate the spherical aberration and astigmatism.

[0060] (a-2) The lens unit g5B may include one or more positive lenses and two or more negative lenses.

[0061] The image stabilizing lens unit g5 has relatively large negative power rather than the entire lens system. The image stabilizing lens unit g5B made of one negative lens would become advantageous in weight, but result in an insufficient optical performance in stabilizing an image. The image stabilizing lens unit g5B made of two of positive and negative lens could easily correct chromatic aberration, but result in a large mobile amount in the direction perpendicular to the optical axis due to the insufficient lens power even in stabilizing an image. Therefore, the lens unit g5B preferably includes at least one positive lens and at least two negative lenses, thereby keeping the large lens power, reducing the moving amount in the direction perpendicular to the optical axis in stabilizing an image, and maintaining the good optical performance.

[0062] (a-3) The front lens component G1 includes, in order from the object side, a first lens unit g1 of positive refractive power, a second lens unit g2 of positive or negative refractive power, a third lens unit g3 of negative refractive power, and a fourth lens unit g4 of positive refractive power, wherein during zooming, a separation between the first and second lens units g1 and g2 is fixed or increases, a separation between the second and third lens units g2 and g3 increases, and a separation between the third and fourth lens units g3 and g4 changes.

[0063] (a-4) The second lens unit may move along the optical axis for focusing.

[0064] (a-5) The first lens unit and the lens unit G2 may not move for zooming.

[0065] (a-6) The following condition may be satisfied where Bf is a distance from an image plane to a vertex in an image-side lens surface of a lens closest to the image, and ft is a focal length of an entire lens system at a telephoto end:

Bf/ft>0.25   (4)

[0066] The equation (4) indicates a ratio of a distance (i.e., a back focus) from a vertex in the image-side surface of the lens closest to the image side to the shot surface relative to the focal distance of the entire lens system at the telephoto end. As the focal distance ft exceeding the lower limit value would make difficult the attachment, for example, between the lens body and the camera body.

[0067] The above structure provides a good image stabilizing function and a good aberrational correction to a zoom lens system, suitable for video camera, video still camera, cameras using a silver halide film etc., which has an angle of field from about 34° to 12°, an F number of about 2.8.

[0068] Next follows a description of a single lens reflex camera (as an optical apparatus) using a zoom lens system as an image pick-up system of an embodiment according to the present invention, with reference to FIG. 25.

[0069] In FIG. 25, 10 denotes a camera body, 11 denotes an image pick-up optical system including the zoom lens of the present invention, 12 denotes an image-taking device (“a photoelectric conversion element”), such as a CCD or a silver halide film, which receives a subject image from the image pick-up optical system 11, 13 denotes a finder system including a focus plate 15 on which a subject image is formed, pentagonal prism 16 as image inversion means, and an eyepiece 17 for observing the subject image on the focus plate 15.

[0070] Thus, an application of the inventive zoom lens system to a camera such as a video camera, a digital still camera, a single lens reflex camera etc., would render small the optical apparatus and enhance the optical performance.

[0071] Next follows numerical data for numerical examples. In each numerical example, “ri” represents a radius of curvature of the i-th surface in order from the object side. “di” represents a thickness of the i-th optical member or a separation of air in order from the object side. “ni” and “vi” are the refractive index and Abbe number of the material of the i-th optical member in order from the object side.

[0072] Each Table shows a relationship between the above equations and various numerical values in the numerical examples.

Numerical Example 1

[0073] f = 72.49805  fno = 1:2.9  2ω = 34.2°˜12.4° r1 = 419.962 d1 = 2.80 n1 = 1.74950 ν1 = 35.3 r2 = 132.534 d2 = 0.23 r3 = 138.957 d3 = 7.52 n2 = 1.49700 ν2 = 81.5 r4 = −407.574 d4 = 0.10 r5 = 90.528 d5 = 6.64 n3 = 1.49700 ν3 = 81.5 r6 = 332.596 d6 = Vari- able r7 = 47.719 d7 = 2.50 n4 = 1.84666 ν4 = 23.8 r8 = 41.657 d8 = 1.82 r9 = 49.949 d9 = 8.77 n5 = 1.48749 ν5 = 70.2 r10 = 6214.652 d10 = Vari- able r11 = 1840.842 d11 = 1.40 n6 = 1.80610 ν6 = 40.9 r12 = 36.505 d12 = 5.55 r13 = −86.160 d13 = 1.40 n7 = 1.48749 ν7 = 70.2 r14 = 38.587 d14 = 5.08 n8 = 1.84666 ν8 = 23.8 r15 = 422.938 d15 = 2.47 r16 = −67.770 d16 = 1.40 n9 = 1.71299 ν9 = 53.9 r17 = 304.729 d17 = Vari- able r18 = 218.633 d18 = 7.01 n10 = 1.49700 ν10 = 81.5 r19 = −34.066 d19 = 1.10 r20 = −32.873 d20 = 1.45 n11 = 1.66680 ν11 = 33.0 r21 = −82.289 d21 = 0.15 r22 = 138.166 d22 = 3.00 n12 = 1.84666 ν12 = 23.8 r23 = ∞ d23 = Vari- able r24 = ∞ Stop d24 = 0.25 r25 = 53.680 d25 = 5.00 n13 = 1.77250 ν13 = 49.6 r26 = 138.666 d26 = 7.32 r27 = 44.371 d27 = 3.00 n14 = 1.84666 ν14 = 23.8 r28 = 23.175 d28 = 0.15 r29 = 23.436 d29 = 7.00 n15 = 1.60311 ν15 = 60.6 r30 = −203.339 d30 = Vari- able r31 = 269.475 d31 = 3.50 n16 = 1.84666 ν16 = 23.8 r32 = −82.499 d32 = 1.35 n17 = 1.69350 ν17 = 53.2 r33 = 31.261 d33 = 3.90 r34 = −66.833 d34 = 1.35 n18 = 1.69350 ν18 = 53.2 r35 = 136.353 d35 = Vari- able r36 = 113.450 d36 = 8.89 n19 = 1.49700 ν19 = 81.5 r37 = −22.151 d37 = 0.50 r38 = −22.027 d38 = 1.80 n20 = 1.83400 ν20 = 37.2 r39 = −49.895 d39 = 4.22 r40 = 117.787 d40 = 4.00 n21 = 1.83400 ν21 = 37.2 r41 = −182.364

[0074] TABLE 1 VARIABLE FOCAL LENGTH SEPARATION 72.50  99.50  194.99  d 6 7.03 13.28  34.81  d 10 1.80 9.85 17.55  d 17 33.14  25.43  0.70 d 23 12.09  5.50 1.00 d 30 2.99 2.99 2.99 d 35 4.79 4.79 4.79

Numerical Example 2

[0075] f = 72.50014  fno = 1:2.9  2ω = 34.2°˜12.4° r1 = 356.432 d1 = 2.80 n1 = 1.80100 ν1 = 35.0 r2 = 105.963 d2 = 0.51 r3 = 115.226 d3 = 5.09 n2 = 1.48749 ν2 = 70.2 r4 = 324.799 d4 = 0.15 r5 = 121.032 d5 = 7.19 n3 = 1.48749 ν3 = 70.2 r6 = −1610.690 d6 = 0.15 r7 = 75.548 d7 = 7.13 n4 = 1.48749 ν4 = 70.2 r8 = 210.911 d8 = Vari- able r9 = 57.175 d9 = 3.00 n5 = 1.78470 ν5 = 26.3 r10 = 45.651 d10 = 1.45 r11 = 51.733 d11 = 9.75 n6 = 1.48749 ν6 = 70.2 r12 = 1094.956 d12 = Vari- able r13 = 212.158 d13 = 1.40 n7 = 1.83481 ν7 = 42.7 r14 = 30.453 d14 = 7.08 r15 = −79.314 d15 = 1.40 n8 = 1.51633 ν8 = 64.1 r16 = 35.144 d16 = 6.61 n9 = 1.84666 ν9 = 23.8 r17 = −4959.330 d17 = 3.19 r18 = −46.447 d18 = 1.40 n10 = 1.77250 ν10 = 49.6 r19 = −281.544 d19 = Vari- able r20 = −696.658 d20 = 6.95 n11 = 1.49700 ν11 = 81.5 r21 = −30.928 d21 = 0.50 r22 = −30.664 d22 = 1.45 n12 = 1.80440 ν12 = 39.6 r23 = −51.445 d23 = 0.15 r24 = 142.742 d24 = 3.22 n13 = 1.83481 ν13 = 42.7 r25 = −424.715 d25 = Vari- able r26 = ∞ Stop d26 = 0.30 r27 = 39.801 d27 = 6.00 n14 = 1.77250 ν14 = 49.6 r28 = 72.709 d28 = 11.28 r29 = 56.870 d29 = 2.00 n15 = 1.78470 ν15 = 26.3 r30 = 22.764 d30 = 0.15 r31 = 23.291 d31 = 6.50 n16 = 1.51633 ν16 = 64.1 r32 = −138.022 d32 = Vari- able r33 = −687.332 d33 = 3.16 n17 = 1.84666 ν17 = 23.8 r34 = −51.923 d34 = 1.00 n18 = 1.66755 ν18 = 41.9 r35 = 52.100 d35 = 2.25 r36 = −182.246 d36 = 1.50 n19 = 1.56873 ν19 = 63.2 r37 = 46.916 d37 = Vari- able r38 = 65.955 d38 = 11.50 n20 = 1.49700 ν20 = 81.5 r39 = −23.351 d39 = 0.15 r40 = −23.857 d40 = 2.00 n21 = 1.87400 ν21 = 35.3 r41 = −55.118 d41 = 3.99 r42 = 66.661 d42 = 5.00 n22 = 1.80518 ν22 = 25.4 r43 = 217.647

[0076] TABLE 2 VARIABLE FOCAL LENGTH SEPARATION 72.50  99.50  195.00  d 8 8.93 9.27 11.58  d 12 0.15 10.75  23.45  d 19 29.97  23.17  0.15 d 25 4.30 0.15 8.16 d 32 3.50 3.50 3.50 d 37 4.81 4.81 4.81

Numerical Example 3

[0077] f = 72.49989  fno = 1:2.9  2ω = 34.2°˜12.4° r1 = 208.784 d1 = 3.00 n1 = 1.80518 ν1 = 25.4 r2 = 99.862 d2 = 0.19 r3 = 100.245 d3 = 8.93 n2 = 1.49700 ν2 = 81.5 r4 = −1100.443 d4 = 0.15 r5 = 112.074 d5 = 6.54 n3 = 1.49700 ν3 = 81.5 r6 = 1249.374 d6 = 0.15 r7 = 92.103 d7 = 7.22 n4 = 1.49700 ν4 = 81.5 r8 = 1027.264 d8 = Varia- able r9 = 593.222 d9 = 1.50 n5 = 1.51633 ν5 = 64.1 r10 = 152.422 d10 = 1.32 r11 = 482.806 d11 = 3.25 n6 = 1.84666 ν6 = 23.8 r12 = −250.113 d12 = 1.50 n7 = 1.62299 ν7 = 58.2 r13 = 94.822 d13 = Vari- able r14 = 261.447 d14 = 1.40 n8 = 1.77250 ν8 = 49.6 r15 = 41.132 d15 = 4.57 r16 = −125.838 d16 = 1.40 n9 = 1.48749 ν9 = 70.2 r17 = 44.165 d17 = 4.62 n10 = 1.84666 ν10 = 23.8 r18 = 777.630 d18 = 2.90 r19 = −52.946 d19 = 1.40 n11 = 1.69895 ν11 = 30.1 r20 = −227.139 d20 = Vari- able r21 = −8791.826 d21 = 2.89 n12 = 1.77250 ν12 = 49.6 r22 = −108.787 d22 = 0.15 r23 = 76.950 d23 = 6.39 n13 = 1.49700 ν13 = 81.5 r24 = −55.536 d24 = 1.45 n14 = 1.83400 ν14 = 37.2 r25 = −362.335 d25 = Vari- able r26 = 56.128 d26 = 3.72 n15 = 1.84666 ν15 = 23.8 r27 = 243.845 d27 = 1.00 r28 = ∞ Stop d28 = 9.68 r29 = 54.942 d29 = 3.44 n16 = 1.80400 ν16 = 46.6 r30 = 334.920 d30 = 0.00 r31 = 334.920 d31 = 1.08 n17 = 1.80518 ν17 = 25.4 r32 = 19.586 d32 = 0.00 r33 = 19.586 d33 = 6.99 n18 = 1.60311 ν18 = 60.6 r34 = −470.040 d34 = Vari- able r35 = 141.442 d35 = 1.40 n19 = 1.83400 ν19 = 37.2 r36 = 44.284 d36 = 2.28 r37 = −116.282 d37 = 1.40 n20 = 1.61772 ν20 = 49.8 r38 = 24.567 d38 = 4.00 n21 = 1.84666 ν21 = 23.8 r39 = 41.388 d39 = Vari- able r40 = 103.965 d40 = 9.35 n22 = 1.63930 ν22 = 44.9 r41 = −24.368 d41 = 0.15 r42 = −24.765 d42 = 1.20 n23 = 1.83481 ν23 = 42.7 r43 = −61.808 d43 = 12.91 r44 = 60.361 d44 = 5.50 n24 = 1.77250 ν24 = 49.6 r45 = 170.890

[0078] TABLE 3 VARIABLE FOCAL LENGTH SEPARATION 72.50  99.78  195.00  d 8 0.15 11.76  21.05  d 13 11.60  12.71  28.25  d 20 31.55  23.97  0.15 d 25 6.29 1.16 0.15 d 34 2.58 2.58 2.58 d 39 4.15 4.15 4.15

Numerical Example 4

[0079] f = 72.52892  fno = 1:2.9  2ω = 34.2°˜12.4° r1 = 113.707 d1 = 2.80 n1 = 1.76180 ν1 = 27.1 r2 = 69.528 d2 = 0.43 r3 = 69.049 d3 = 12.74 n2 = 1.49700 ν2 = 81.5 r4 = −308.469 d4 = 0.10 r5 = 73.095 d5 = 7.94 n3 = 1.49700 ν3 = 81.5 r6 = 392.342 d6 = Vari- able r7 = 979.779 d7 = 2.96 n4 = 1.80809 ν4 = 22.8 r8 = −254.050 d8 = 1.40 n5 = 1.65160 ν5 = 58.5 r9 = 87.091 d9 = Vari- able r10 = 153.160 d10 = 1.40 n6 = 1.72825 ν6 = 28.5 r11 = 36.920 d11 = 4.88 r12 = −130.193 d12 = 1.40 n7 = 1.48749 ν7 = 70.2 r13 = 38.438 d13 = 5.24 n8 = 1.84666 ν8 = 23.8 r14 = 960.814 d14 = 2.88 r15 = −52.962 d15 = 1.40 n9 = 1.72600 ν9 = 53.6 r16 = −1060.876 d16 = Vari- able r17 = 6450.021 d17 = 2.50 n10 = 1.81554 ν10 = 44.4 r18 = −154.954 d18 = 0.15 r19 = 139.424 d19 = 6.11 n11 = 1.49700 ν11 = 81.5 r20 = −46.016 d20 = 1.45 n12 = 1.80100 ν12 = 35.0 r21 = −124.015 d21 = Vari- able r22 = 51.975 d22 = 3.56 n13 = 1.84666 ν13 = 23.8 r23 = 138.077 d23 = 1.50 r24 = ∞ Stop d24 = 8.60 r25 = 40.516 d25 = 3.14 n14 = 1.78800 ν14 = 47.4 r26 = 74.677 d26 = 0.00 r27 = 74.675 d27 = 1.00 n15 = 1.80809 ν15 = 22.8 r28 = 21.524 d28 = 0.00 r29 = 21.394 d29 = 7.50 n16 = 1.58913 ν16 = 61.1 r30 = −195.490 d30 = Vari- able r31 = 386.103 d31 = 1.40 n17 = 1.80100 ν17 = 35.0 r32 = 43.907 d32 = 2.09 r33 = −264.153 d33 = 1.40 n18 = 1.58875 ν18 = 51.2 r34 = 22.280 d34 = 4.00 n19 = 1.84666 ν19 = 23.8 r35 = 32.432 d35 = Vari- able r36 = 62.047 d36 = 11.62 n20 = 1.60323 ν20 = 42.3 r37 = −21.742 d37 = 0.18 r38 = −21.336 d38 = 1.20 n21 = 1.83481 ν21 = 42.7 r39 = −88.906 d39 = 8.51 r40 = 71.082 d40 = 5.50 n22 = 1.72600 ν22 = 53.6 r41 = −1405.961

[0080] TABLE 4 FOCAL LENGTH 72.53  99.47 194.97  d 6 0.45 11.63 21.63  d 9 11.28  12.97 26.71  d 16 30.85  23.88 0.15 d 21 6.11  0.20 0.20 d 30 2.78  2.78 2.78 d 35 4.15  4.15 4.15

[0081] TABLE 5 NUMERICAL EXAMPLE EQUATIONS Example 1 Example 2 Example 3 Example 4 (1) f5A/f5B −1.738 −1.902 −1.790 −1.583 (2) f5C/f5B −1.970 −1.643 −1.589 −1.977 (3) f5B/fw −0.413 −0.523 −0.456 −0.405 (4) Bf/ft  0.310  0.289  0.271  0.269

[0082] Thus, the present embodiment may provide a zoom lens system and optical apparatus using the same, where the zoom lens has a large aperture but provides an image stabilizing system that has a small and lightweight image stabilizing lens unit, providing a good optical performance even in stabilizing an image and making compact the entire apparatus.

[0083] In addition, the present embodiment may provide a large-aperture zoom lens system where the rear lens component including a relay lens part in the above structure includes a positive lens unit, a negative lens unit (or image stabilizing lens unit), and a positive lens unit, thereby achieving suitable image stabilizing function and a high optical performance by moving the negative lens unit in the relay lens part in the direction perpendicular to the optical axis in correcting an image plane while stabilizing an image. 

What is claimed is:
 1. A zoom lens system comprising, in order from an object side: a front lens component including a plurality of lens units for zooming and focusing; and a rear lens component unit for forming an image, wherein said rear lens component including, in order from the object side, a lens unit A of positive refractive power, a lens unit B of negative refractive power movable so as to have a component in a direction perpendicular to an optical axis for displacing the image, and a lens unit C of positive refractive power, the image being displaced as the lens unit B moves so as to have the component in the direction perpendicular to an optical axis.
 2. A zoom lens system according to claim 1, wherein conditions −2.5<f5A/f5B<−1.0, 2.5<f5C/f5B<−1.0, and −1.0<f5B/fw<−0.1 are satisfied where f5A, f5B, and f5C are focal lengths of said lens units A, B and C, respectively, and fw is a focal length of an entire lens system at wide-angle end.
 3. A zoom lens system according to claim 1, wherein said lens unit B includes one or more positive lenses, and two or more negative lenses.
 4. A zoom lens system according to claim 1, wherein said front lens component includes, in order from the object side: a first lens unit of positive refractive power; a second lens unit of positive or negative refractive power; a third lens unit of negative refractive power; and a fourth lens unit of positive refractive power, wherein during zooming from a wide-angle end to a telephoto end, a separation between the first and second lens units keeps constant or increases, a separation between the second and third lens units increases, and a separation between the third and fourth lens units changes.
 5. A zoom lens system according to claim 4, wherein said second lens unit moves along the optical axis during focusing.
 6. A zoom lens system according to claim 4, wherein said first lens unit and rear lens component don't move for zooming.
 7. A zoom lens system according to claim 1, wherein a condition Bf/ft>0.25 is satisfied where Bf is a distance from an image plane to a vertsx in a lens surface at an image side of a lens closest to the image, and ft is a focal length of an entire lens system at a telephoto end.
 8. An optical apparatus comprising: a zoom lens system comprising, in order from an object side, a front lens component including a plurality of lens units for zooming and focusing, and a rear lens component for forming an image, wherein said rear lens component including, in order from the object side, a lens unit A of positive refractive power, a lens unit B of negative refractive power movable so as to have a component in a direction perpendicular to an optical axis for displacing the image, and a lens unit C of positive refractive power, the image being displaced as the lens unit B moves so as to have the component in the direction perpendicular to an optical axis; and a photoelectric conversion element for receiving an image formed by said zoom lens system. 